# Using the single template model¶

The single template model is useful for when you know all the intrinsic parameters of your signal (say the masses, spins, etc of a merger). In this case, we don’t need to recalculate the waveform model to sample different possible extrinsic parameters (i.e. distance, sky location, inclination). This can greatly speed up the calculation of the likelihood. To use this model you provide the intrinsic parameters as fixed arguments as in the configuration file below.

This example demonstrates using the single_template model with the emcee_pt sampler. First, we create the following configuration file:

[model]
name = single_template

#; This model precalculates the SNR time series at a fixed rate.
#; If you need a higher time resolution, this may be increased
sample_rate = 32768
low-frequency-cutoff = 30.0
no-save-data =

[data]
instruments = H1 L1 V1
analysis-start-time = 1187008482
analysis-end-time = 1187008892
psd-estimation = median
psd-segment-length = 16
psd-segment-stride = 8
psd-inverse-length = 16
channel-name = H1:LOSC-STRAIN L1:LOSC-STRAIN V1:LOSC-STRAIN
frame-files = H1:H-H1_LOSC_CLN_4_V1-1187007040-2048.gwf L1:L-L1_LOSC_CLN_4_V1-1187007040-2048.gwf V1:V-V1_LOSC_CLN_4_V1-1187007040-2048.gwf
strain-high-pass = 15
sample-rate = 2048

[sampler]
no-save-state =
name = dynesty
nlive = 500
walks = 100
maxmcmc = 500
nact = 10
sample = rwalk2

[sampler-burn_in]
burn-in-test = min_iterations
min-iterations = 100

[variable_params]
; waveform parameters that will vary in MCMC
tc =
distance =
inclination =

[static_params]
; waveform parameters that will not change in MCMC
approximant = TaylorF2
f_lower = 30
mass1 = 1.3757
mass2 = 1.3757

#; we'll choose not to sample over these, but you could
polarization = 0
ra = 3.44615914
dec = -0.40808407

#; You could also set additional parameters if your waveform model supports / requires it.
; spin1z = 0

[prior-tc]
; coalescence time prior
name = uniform
min-tc = 1187008882.4
max-tc = 1187008882.5

[prior-distance]
#; following gives a uniform in volume
min-distance = 10
max-distance = 60

[prior-inclination]
name = sin_angle


Download

for ifo in H-H1 L-L1 V-V1
do
file=${ifo}_LOSC_CLN_4_V1-1187007040-2048.gwf test -f${file} && continue
curl -O --silent https://dcc.ligo.org/public/0146/P1700349/001/${file} done  By setting the model name to single_template we are using SingleTemplate. Now run: pycbc_inference \ --config-file dirname "$0"/single.ini \
--nprocesses=4 \
--output-file single.hdf \
--seed 0 \
--force \
--verbose


Download

This will run the emcee_pt sampler. When it is done, you will have a file called single.hdf which contains the results. It should take about a minute or two to run.

To plot the posterior distribution after the last iteration, run:

pycbc_inference_plot_posterior \
--input-file single.hdf \
--output-file single.png \
--z-arg snr


Download

This will create the following plot:

The scatter points show each walker’s position after the last iteration. The points are colored by the log likelihood at that point, with the 50th and 90th percentile contours drawn.

The single template model also supports marginalization over the polarization angle by numerical sampling. The following example features two adanced options. This marginalization and also arbitrary sampling coordinates with nested samplers using the fixed_samples distribution. Here we sample in the time delay space rather than sky location directly.

[model]
name = single_template

#; This model precalculates the SNR time series at a fixed rate.
#; If you need a higher time resolution, this may be increased
sample_rate = 32768
low-frequency-cutoff = 30.0
polarization_samples = 100

[data]
instruments = H1 L1 V1
analysis-start-time = 1187008482
analysis-end-time = 1187008892
psd-estimation = median
psd-segment-length = 16
psd-segment-stride = 8
psd-inverse-length = 16
channel-name = H1:LOSC-STRAIN L1:LOSC-STRAIN V1:LOSC-STRAIN
frame-files = H1:H-H1_LOSC_CLN_4_V1-1187007040-2048.gwf L1:L-L1_LOSC_CLN_4_V1-1187007040-2048.gwf V1:V-V1_LOSC_CLN_4_V1-1187007040-2048.gwf
strain-high-pass = 15
sample-rate = 2048

[sampler]
name = dynesty
nlive = 100

[sampler-burn_in]
burn-in-test = min_iterations
min-iterations = 100

[variable_params]
; waveform parameters that will vary in MCMC
tc =
distance =
inclination =
dh =
dhl =

[static_params]
; waveform parameters that will not change in MCMC
approximant = TaylorF2
f_lower = 30
mass1 = 1.3757
mass2 = 1.3757
#polarization = 0

[prior-tc]
; coalescence time prior
name = uniform
min-tc = 1187008882.4
max-tc = 1187008882.5

[prior-distance]
#; following gives a uniform in volume
min-distance = 10
max-distance = 60

[prior-inclination]
name = sin_angle

[prior-dh+dhl]
name = fixed_samples
subname = mysky
sample-size = 1e6

[mysky_sample-ra+dec]
name = uniform_sky

[mysky_transform-dh+dhl]
name = custom
inputs = ra, dec
dh = det_tc('H1', ra, dec, 1187008882.0, relative=1)
dhl = det_tc('L1', ra, dec, 1187008882.0, relative=1) - det_tc('H1', ra, dec, 1187008882.0, relative=1)

[waveform_transforms-ra+dec]
name = mysky